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Featured researches published by S. C. Chase.


Journal of Geophysical Research | 1992

Thermal emission spectrometer experiment: Mars Observer mission

Philip R. Christensen; Don L. Anderson; S. C. Chase; Roger N. Clark; Hugh H. Kieffer; Michael C. Malin; John C. Pearl; James Carpenter; Nuno Bandiera; F. Gerald Brown; Steven H. Silverman

Thermal infrared spectral measurements will be made of the surface and atmosphere of Mars by the thermal emission spectrometer (TES) on board Mars Observer. By using these observations the composition of the surface rocks, minerals, and condensates will be determined and mapped. In addition, the composition and distribution of atmospheric dust and condensate clouds, together with temperature profiles of the CO2 atmosphere, will be determined. Broadband solar reflectance and thermal emittance measurements will also be made to determine the energy balance in the polar regions and to map the thermophysical properties of the surface. The specific science objectives of this investigation are to determine (1) the composition and distribution of surface materials, (2) the composition, particle size, and spatial and temporal distribution of suspended dust, (3) the location, temperature, height, and water abundance of H2O clouds, (4) the composition, seasonal behavior, total energy balance, and physical properties of the polar caps, and (5) the particle size distribution of rocks and fines on the surface. The instrument consists of three subsections: a Michelson interferometer, a solar reflectance sensor, and a broadband radiance sensor. The spectrometer covers the wavelength range from 6 to 50 μm (∼1600–200 cm−1) with nominal 5 and 10 cm−1 spectral resolution. The solar reflectance band extends from 0.3 to 2.7 μm; the broadband radiance channel extends from 5.5 to 100 μm. There are six 8.3-mrad fields of view for each sensor arranged in a 3 × 2 array, each with 3-km resolution at the nadir. Uncooled deuterated triglycine sulphate (DTGS) pyroelectic detectors provide a signal-to-noise ratio (SNR) of over 500 at 10 μm for daytime spectral observations at a surface temperature of 270 K. The SNR of the albedo and thermal bolometers will be approximately 2000 at the peak signal levels expected. The instrument is 23.6 × 35.5 × 40.0 cm, with a mass of 14.4 kg and an average power consumption of 14.5 W. The approach will be to measure the spectral properties of thermal energy emitted from the surface and atmosphere. Emission phase angle studies and day-night observations will be used to separate the spectral character of the surface and atmosphere. The distinctive thermal infrared spectral features present in minerals, rocks, and condensates will be used to determine the mineralogic and petrologic character of the surface and to identify and study aerosols and volatiles in the atmosphere.


Science | 1976

Martian North Pole Summer Temperatures: Dirty Water Ice

Hugh H. Kieffer; S. C. Chase; Terry Z. Martin; E. D. Miner; Frank D. Palluconi

Broadband thermal and reflectance observations of the martian north polar region in late summer yield temperatures for the residual polar cap near 205 K with albedos near 43 percent. The residual cap and several outlying smaller deposits are water ice with included dirt; there is no evidence for any permanent carbon dioxide polar cap.


Science | 1976

Infrared Thermal Mapping of the Martian Surface and Atmosphere: First Results

Hugh H. Kieffer; S. C. Chase; E. D. Miner; Frank D. Palluconi; G. Münch; G. Neugebauer; Terry Z. Martin

The Viking infrared thermal mapper measures the thermal emission of the martian surface and atmosphere and the total reflected sunlight. With the high resolution and dense coverage being achieved, planetwide thermal structure is apparent at large and small scales. The thermal behavior of the best-observed areas, the landing sites, cannot be explained by simple homogeneous models. The data contain clear indications for the relevance of additional factors such as detailed surface texture and the occurrence of clouds. Areas in the polar night have temperatures distinctly lower than the CO2 condensation point at the surface pressure. This observation implies that the annual atmospheric condensation is less than previously assumed and that either thick CO2 clouds exist at the 20-kilometer level or that the polar atmosphere is locally enriched by noncondensable gases.


Science | 1980

Pioneer Saturn Infrared Radiometer: Preliminary Results

A. P. Ingersoll; Glenn S. Orton; G. Münch; G. Neugebauer; S. C. Chase

The effective temperature of Saturn, 94.4 + 3 K, implies a total emission greater than two times the absorbed sunlight. The infrared data alone give an atmospheric abundance of H2 relative to H2 + He of 0.85 � 0.15. Comparison of infrared and radio occultation data will give a more precise estimate. Temperature at the 1-bar level is 137 to 140 K, and 2.5 K differences exist between belts and zones up to the 0.06-bar level. Ring temperatures range from 60 to 70 K on the south (illuminated) side and from < 60 to 67 K in the planets shadow. The average temperature of the north (unilluminated) side is ∼ 55 K. Titans 45-micrometer brightness temperature is 80 � 10 K.


Icarus | 1976

Mariner 10 infrared radiometer results: Temperatures and thermal properties of the surface of Mercury

S. C. Chase; E. Miner; David Morrison; G. Münch; G. Neugebauer

Mariner 10 infrared brightness temperatures of the surface of Mercury at 11 and 45 μm are presented. The data were obtained during the first flyby along a nera-equatorial swath extending from 17 hours local time through local midnight to 9 hours local time. For an assumed emissivity of 0.9, derived surface thermal inertias are between 0.0031 and 0.0031 cal cm^(−2)sec^(−12) K^(−1) and the implied minimum predawn surface kinetic temperature for the warm pole at longitude 270° is near 93 K. Several pronounced thermal inhomogeneities were seen, one of which appears to coincide with a region of high radar reflectivity. The derived thermal properties and the electrical skin depth and loss tangent fall within the range of values found on the Moon.


Applied Optics | 1978

Viking infrared thermal mapper

S. C. Chase; Jack L. Engel; Howard W. Eyerly; Hugh H. Kieffer; Frank D. Palluconi; Donald Schofield

The infrared thermal mapper (IRTM) was designed to measure the emitted and reflected radiance of Mars. Carried by the Viking Orbiter, the IRTM contains four small Cassegrainian telescopes which each image the same, seven circular areas. There is a total of twenty-eight channels in four surface and one atmospheric thermal bands from 6 microm to 30 microm and a broad solar reflectance band. All channels are sampled simultaneously, using the spacecraft scanning capability to map the radiance over small and large areas of the planet. All channels use thermopile detectors; spectral passbands are determined by a combination of interference filters, detector lense materials, antireflection coatings, and restrahlen optics.


Science | 1974

Pioneer 10 Infrared Radiometer Experiment: Preliminary Results

S. C. Chase; R. D. Ruiz; G. Münch; G. Neugebauer; M. Schroeder; Laurence M. Trafton

Thermal maps of Jupiter at 20 and 40 micrometers show structure closely related to the visual appearance of the planet. Peak brightness temperatures of 126� and 145�K have been measured on the South Equatorial Belt, for the 20- and 40-micrometer channels, respectively. Corresponding values for the South Tropical Zone are 120� and 138�K. No asymmetries between the illuminated sunlit and nonilluminated parts of the disk were found. A preliminary discussion of the data, in terms of simple radiative equilibrium models, is presented. The net thermal energy of the planet as a whole is twice the solar energy input.


Science | 1975

Pioneer 11 Infrared Radiometer Experiment: The Global Heat Balance of Jupiter

A. P. Ingersoll; G. Münch; G. Neugebauer; D. J. Diner; Glenn S. Orton; B. Schupler; M. Schroeder; S. C. Chase; R. D. Ruiz; Laurence M. Trafton

Data obtained by the infrared radiometers on the Pioneer 10 and Pioneer 11 spacecraft, over a large range of emission angles, have indicated an effective temperature for Jupiter of 125� � 3�K. The implied ratio of planetary thermal emission to solar energy absorbed is 1.9�0.2, a value not significantly different from the earth-based estimate of 2.5�0.5.


Science | 1969

Mariner 1969: preliminary results of the infrared radiometer experiment.

G. Neugebauer; G. Münch; S. C. Chase; H. Hatzenbeler; E. Miner; D. Schofield

The thermal energy emitted by Mars was measured in the 8- to 12- and 18- to 25-micrometer bands. The minimum temperature derived for the southern polar cap is 150�K, an indication that the cap is formed by frozen carbon dioxide. No significant temperature fluctuations were detected with a 100-kilometer scale.


Icarus | 1972

Infrared thermal mapping experiment: The Viking Mars orbiter

Hugh H. Kieffer; G. Neugebauer; G. Münch; S. C. Chase; E. Miner

The Mars infrared thermal mapper (IRTM) will be carried on the scan platform of the orbiter of the Viking 1975 mission. The IRTM is a multichannel radiometer with several detectors in each of six spectral regions. This instrument will measure the reflected solar radiation and surface thermal emission from the area viewed by the orbiter imaging system with nominal 5 km resolution. Extensive additional areas will be covered for which simultaneous imaging will not be available. The spectral channels are selected to be sensitive to surface emissivity variations and provide good temperature resolution over the entire range of Martian temperatures. These observations will allow determination of the surface kinetic temperature and thermal balance, and by coverage of the dark hemisphere, a search for regions with anomalous cooling can be made. Observations of ground frosts or clouds will help to determine their composition, and in the case of extensive H_2O frosts, will allow the local water vapor pressure to be estimated.

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G. Münch

California Institute of Technology

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Hugh H. Kieffer

United States Geological Survey

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E. Miner

Jet Propulsion Laboratory

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E. D. Miner

California Institute of Technology

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Frank D. Palluconi

California Institute of Technology

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A. P. Ingersoll

California Institute of Technology

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Glenn S. Orton

California Institute of Technology

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M. Schroeder

California Institute of Technology

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